EP0425088B1 - Information storage in holograms - Google Patents
Information storage in holograms Download PDFInfo
- Publication number
- EP0425088B1 EP0425088B1 EP90310133A EP90310133A EP0425088B1 EP 0425088 B1 EP0425088 B1 EP 0425088B1 EP 90310133 A EP90310133 A EP 90310133A EP 90310133 A EP90310133 A EP 90310133A EP 0425088 B1 EP0425088 B1 EP 0425088B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- pixel light
- light beams
- information
- pixel
- array
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired - Lifetime
Links
- 230000000295 complement effect Effects 0.000 claims description 22
- 238000000034 method Methods 0.000 claims description 12
- 230000004044 response Effects 0.000 claims description 4
- 238000006073 displacement reaction Methods 0.000 claims description 2
- 238000003491 array Methods 0.000 claims 4
- 230000003287 optical effect Effects 0.000 description 10
- 239000013078 crystal Substances 0.000 description 8
- 238000012545 processing Methods 0.000 description 5
- 230000000694 effects Effects 0.000 description 4
- 230000006870 function Effects 0.000 description 4
- 239000013598 vector Substances 0.000 description 3
- 101100234408 Danio rerio kif7 gene Proteins 0.000 description 2
- 101100221620 Drosophila melanogaster cos gene Proteins 0.000 description 2
- 101100007330 Saccharomyces cerevisiae (strain ATCC 204508 / S288c) COS2 gene Proteins 0.000 description 2
- 101100398237 Xenopus tropicalis kif11 gene Proteins 0.000 description 2
- 230000001427 coherent effect Effects 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 238000012805 post-processing Methods 0.000 description 2
- 230000005540 biological transmission Effects 0.000 description 1
- JSILWGOAJSWOGY-UHFFFAOYSA-N bismuth;oxosilicon Chemical compound [Bi].[Si]=O JSILWGOAJSWOGY-UHFFFAOYSA-N 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000003760 hair shine Effects 0.000 description 1
- 230000001939 inductive effect Effects 0.000 description 1
- 230000002452 interceptive effect Effects 0.000 description 1
- 239000004973 liquid crystal related substance Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
Images
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
- G03H1/02—Details of features involved during the holographic process; Replication of holograms without interference recording
- G03H1/024—Hologram nature or properties
- G03H1/0248—Volume holograms
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03H—HOLOGRAPHIC PROCESSES OR APPARATUS
- G03H1/00—Holographic processes or apparatus using light, infrared or ultraviolet waves for obtaining holograms or for obtaining an image from them; Details peculiar thereto
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11B—INFORMATION STORAGE BASED ON RELATIVE MOVEMENT BETWEEN RECORD CARRIER AND TRANSDUCER
- G11B7/00—Recording or reproducing by optical means, e.g. recording using a thermal beam of optical radiation by modifying optical properties or the physical structure, reproducing using an optical beam at lower power by sensing optical properties; Record carriers therefor
- G11B7/004—Recording, reproducing or erasing methods; Read, write or erase circuits therefor
- G11B7/0065—Recording, reproducing or erasing by using optical interference patterns, e.g. holograms
-
- G—PHYSICS
- G11—INFORMATION STORAGE
- G11C—STATIC STORES
- G11C13/00—Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00
- G11C13/04—Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00 using optical elements ; using other beam accessed elements, e.g. electron or ion beam
- G11C13/042—Digital stores characterised by the use of storage elements not covered by groups G11C11/00, G11C23/00, or G11C25/00 using optical elements ; using other beam accessed elements, e.g. electron or ion beam using information stored in the form of interference pattern
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S359/00—Optical: systems and elements
- Y10S359/90—Methods
Definitions
- the present invention relates to holographic apparatus for storage and retrieval of information and to methods of information storage and retrieval using such holographic apparatus.
- monochromatic light beams impinging upon photorefractive mediums such as bismuth silicon oxide (BSO)
- BSO bismuth silicon oxide
- the light interference results in storage of data carried by the light beams as a volume hologram in a portion of the medium.
- Readout of the stored hologram is achieved by shining a reference light beam into the medium, causing the reference beam to be modulated by the stored hologram as it passes through the medium and leaves the medium along an output light path.
- a thick photorefractive medium such as BSO.
- the stored hologram is readable by a readout reference beam aligned at the same angle of incidence used for recording the respective superimposed holograms.
- Such recording has required that the intensity of the pixels in the hologram is modulated to carry information. This use of intensity modulation is particularly subject to noise introduced into the signal by the optical paths of the light beams.
- a laser monochromatic light beam in addition to carrying information based upon light intensity modulation, can carry information by means of differing angles of rotation of the plane of linear polarisation of the light beam with respect to a reference plane of linear light polarisation.
- Such rotation of the plane of polarisation results in P and S components, which are orthogonally disposed in the light beam.
- An example of such modulation is the readback light beam reflected from or transmitted through a magneto-optic record medium.
- the readback optics and electrical circuits for a magneto-optic record medium process the P and S components of the modulated reflected light beam for generating modulated output electrical signals wherein the modulations represent the information carried in the P and S components or rotated linear polarisation planes of such monochromatic laser light.
- U. S. Patent 3,825,316 discloses a holographic system in which the polarisation of the light is switched in either of two directions for detection.
- a laser produces a beam of polarised coherent light which is transmitted through a polarisation switching device that adjusts, in response to an input signal, the orientation of the plane of polarisation of the transmitted light in either one of two mutually orthogonal states.
- the light transmitted by the polarisation switching device then impinges on a transparent electro-optic photorefractive crystaline material whose index of refraction along its C axis varies in accordance with the interference fringes of a pre-established holographic pattern.
- the optical system includes an electro-optic beam deflector to provide a strong polarisation dependent digital laser beam deflection system such that the beam is deflected in a different predetermined direction depending upon the polarisation state of the beam, i.e. beam splitting.
- the optical system includes a complex optical component to provide light deflection apparatus for selectively deflecting a beam of light from a source to one of a plurality of target positions.
- the invention relates to a method of storing and retrieving information in a holographic record medium comprising the steps of: providing an incident pixel array of light beams using substantially linearly polarised monochromatic light having a single reference angle of linear polarisation for all of the pixel light beams; modulating the pixel light beams by rotating the linear polarisations of the respective pixel light beams in response to supplied information so that the information is represented by the respective angles of rotation of the linear polarisations of the light beams; shining a reference beam onto the holographic record medium; and directing the modulated pixel light beams as an array into said record medium and thereby into interference with the reference beam whereby the resultant interference pattern is recorded as a holographic image in the holographic record medium.
- the invention relates to storing in a holographic medium, preferably as a volume hologram, information represented by any one of a plurality of angles of rotation of the plane of linear polarisation having two or more discrete angles of rotation from a reference plane of linear polarisation. All of the polarisation rotations are measured in the same rotational sense.
- a light beam carrying information in the form of a plurality of angular rotational modulations of the plane of linear polarisation of a light beam, is stored as a plurality of images in a photorefractive medium.
- the storage of the images is arranged to be complementary so that imperfections in the medium are compensated for by the complementary storage.
- the modulated light beams are stored as two different images having respective angular modulations separated by ninety degrees, i.e. orthogonal, as measured in a first or rotational direction from a reference plane of linear polarisation.
- signal processing within the storage system introduces the control of the polarisation rotation so that this rotation represents an input signal.
- the output signal of the two images are then divided one into another to produce a single modulated electrical output signal.
- the output signal is a faithful reproduction of the input modulation of a light beam. More than two images may be generated with the divisional function being applied between various pairs of the output signals.
- the invention provides information storage and retrieval apparatus comprising: a source of substantially linearly polarised incident monochromatic light; means for generating from source an array of pixel light beams, all having a single reference angle of linear polarisation; means for selectively modulating the individual pixel light beams in accordance with supplied information so that the information is represented by the angular displacement of the plane of linear polarisation; a holographic record medium located to receive said array of modulated pixel light beams; and means for generating a reference beam and for directing said reference beam to interact with said modulated beams, the angle of linear polarisation of said reference beam being selected so as to generate an interference pattern with said modulated beams, thereby to record holographic images in said medium representing said array of modulated pixel light beams; characterized by further comprising means (15) for rotating the linear polarisations of all the said modulated pixel light beams by substantially 90° in the same rotational direction in order to form a complementary array of modulated pixel light beams
- a photorefractive recording medium 10 such as BSO, is capable of storing volume holograms in superimposed relationships, that is, a plurality of holograms are stored in the same volume portion of the recording medium 10.
- a laser 11 supplies a linearly polarised monochromatic light beam along a path 12 for flooding an input surface of an LCD (liquid crystal device) transmissive array 13.
- Input data supplied along line 14 controls the transmissive array 13 in the modulation of the laser 11 emitted linearly polarised light.
- the arrangement is such that at each pixel position in the array, the uniformly polarised light has its plane of linear polarisation rotated in a first rotational direction through an angle representative of the input data.
- One of the pixels in the array may be designated as a reference pixel, i.e. is not modulated. This enables a relative angular measurement between all of the data carrying pixels and the reference pixels.
- the light transmitted through array 13 is selectively passed through a one-half wave plate 15, also termed a phase plate.
- phase plate 15 When phase plate 15 is in the light path, all of the linear polarisation modulations in the light beam are rotated by ninety degrees.
- phase plate 15 When phase plate 15 is removed from the light path, as indicated by double headed arrow 16, then no rotation of the linear polarisation occurs.
- the phase plate may be positioned in the path of the linearly polarised monochromatic light beam 12 to achieve the same effect.
- the selective phase plate rotation of the linear polarisation planes enables two complementary holographic images to be stored in BSO crystal 10; one holographic image that is not complementarily rotated and a second which is stored with its plane of linear polarisation rotated by 90 degrees.
- a plurality of phase plates may be inserted onto a rapidly rotating circular disk, much like a tachometer disk, such that alternate areas on the disk rotate the light beam polarisation by ninety degrees with the intermediate areas not rotating the light beam. That is, the rotating disk has a plurality of circumferentially spaced-apart phase plates. As the disk rotates, the light beam is transmitted, with no rotation of the plane of polarisation, through the intermediate area and alternatively with 90 degrees rotation through the phase plate area.
- Other arrangements, including electrically actuated rotations may be employed for achieving the construction of two complementary holograms.
- the modulated light passes through a polariser 17, then impinges upon the input surface of BSO record medium 10.
- a reference beam 20 is supplied to the input surface of the BSO crystal 10 to record the modulated light beam as a volume hologram.
- the non-phase plate rotated beam is first recorded in the BSO crystal, then the phase plate 15 moves into optical interceptive relationship to the laser beam to rotate the laser beam creating a complementary volume hologram in the BSO crystal 10.
- the reference beam 20 is rotated to impinge on the BSO crystal 10 at an orthogonal angle of polarisation relative to that at which the first hologram was recorded.
- reference beam 20 may be rotated such that different angles of incidence on the input surface of BSO crystal 10 are achieved.
- reference beam 20 shines upon the input surface of BSO crystal 10 without any input from laser 11.
- the reference beam is positioned at an angle to read the first hologram.
- the first hologram modulates the reference beam to supply an output set of laser beams (these beams are a reconstructed image of the stored information) which impinge upon an array of detectors 21.
- the second (complementary) hologram was stored at an orthogonal polarisation from the first hologram.
- the reference beam is rotated to the orthogonal polarisation; the read out (reconstruction) proceeds as described for the first hologram.
- the two reconstructed images are sequentially supplied to detectors 21 and therefore are sequentially supplied to read data circuits 22.
- read data circuits 22 supply an output signal through cable 23 by combining the two images through a divisional processing circuit for reconstructing the information carried by the modulation imposed upon the light beam in transmissive array 13.
- Output data (electrical signals) indicated by output cable 23, as will be later described, provide more faithful information reproduction.
- FIG 2 illustrates an advantage of the present invention.
- a first angle of rotation represented by the arrow 26 represents the encoding of input data.
- the arrow is shown to have two lengths 27, 28 which respectively represent two unintended intensity levels of the laser beam.
- this information is stored as two complementary images.
- the first image without the phase plate, stores an image whose intensity is determined by the length of the component 27X or 28X of the arrow 26 two image intensities.
- a phase plate is inserted into the beam, the reference angle is rotated to the orthogonal polarisation, and a second image is recorded.
- phase plate The function of the phase plate is to rotate the arrows (representing the polarisation) by 90 degrees, so that the second image stored now records projections 27Y and 28Y, respectively, for the two intensities of the laser beam.
- the ratio stored y component over stored x component is the tangent of the angle ⁇ enabling the angle ⁇ to be determined. If this process were to occur under different intensity conditions as represented by numerals 27 and 28, there is no noise effect on the information retrieval. In this manner, the described storage process provides insensitivity to unintended variations in light intensity.
- Fig 3 illustrates, in diagrammatic form, a polarisation rotation reference system for faithfully indicating the recorded information.
- a centrally located pixel 30 is unmodulated and therefore represents the reference polarisation location for all of the pixels in the array being stored.
- Each data carrying pixel, such as pixel 31 (there are many such data carrying pixels), is modulated in accordance with the input data on line 14. From Fig 3 it is apparent that if an optical element causes an unintended rotation of the linear polarisation of the multi-pixel light beam, then such unintended linear polarisation rotation will be substantially constant through out the beam and hence, can be accomodated through the use of a reference pixel 30.
- Fig 4 illustrates angular representation of information at a single pixel.
- Six different angles of rotation are shown, all being in a counterclockwise rotational sense from a reference angle of rotation R.
- the various vectors, D1-D6 represent the six angular positions.
- Such six angular positions of rotated linear polarisations can be encoded to represent six different bits, can be a number to the base six, or can be a encoded number in binary form to the sixth power.
- the length of the arrows represents the vector intensity which, of course, is projected by the polariser onto one of the two coordinate axes.
- the angular rotations can extend from zero up to and including 90 degrees.
- Fig 5 shows an embodiment of data read circuits 22 for detecting the information carried on input data line 14 from the volume hologram stored in record medium 10.
- This figure illustrates a so-called post processing arrangement for introducing the arc tangent of square root parameter into the signal detection processing.
- Electrical signals from detectors 21 are in array form, Fig 5 illustrates only one circuit for one pixel.
- a signal from a detector 21 is supplied through an electronic switch 33.
- the first image reconstructed by the reference beam 20 is supplied to a memory M 34. Switch 33 then moves to the alternate terminal to enable processing of the second or complementary signal.
- circuits When the second image is reconstructed by reference beam 20, circuits (not shown) actuate the switch 33 in synchronism with the transmission of the electrical signal from the same detector 21 such that the signals on lines 35 and 36, respectively, represent electrical signals derived from the first and second (complementary) image pixels of the recording medium 10.
- Divide circuit 37 which may be either analog or digital, divides the signal Py, the first recorded signal with no complementary rotation, by the second signal Px, which represents the stored signal rotated by ninety degrees through phase plate 15.
- the output signal of divide circuit 37 carries the electrically modulated signal representative of TAN2 ⁇ on line 38.
- Circuit elements 40 and 41 introduce the arc tangent of square root into the read back signal for producing a signal on line 23′, which is a true reproduction of the input modulation carried by input data on line 14. Final reproduction of the data is provided by a lookup table (not shown) storing values representing the above-described function.
- Circuit 40 is a typical square root circuit, while circuit 41 is a typical arctan circuit.
- the letter "P" indicates the stored pattern or hologram. Note that the signal is embodied in ⁇ (x,y) not in I (x,y) which in general suffers from non-uniformities in the laser, the optical path, and the storage medium. Upon readout, information further unintended intensity non-uniformities may be produced. Thus the patterns read out may be of the form in equations (3) and (4).
- Px′ (x,y) I′(x,y) COS2 ⁇ (x,y)
- Py′ (x,y) I′(x,y) SIN2 ⁇ (x,y)
- the two images are divided into each other on a pixel-by-pixel basis yielding an intermediate result, as represented by the signal on line 38.
- This output signal is independent of any noise in I′ (x,y) induced into the reconstructed patterns.
- the post processing shown in Fig 5 of the square root and arctangent yields a modulated electrical signal carrying the information.
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Holo Graphy (AREA)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US07/425,078 US5039182A (en) | 1989-10-23 | 1989-10-23 | Storing information in dual holographic images |
US425078 | 1989-10-23 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0425088A2 EP0425088A2 (en) | 1991-05-02 |
EP0425088A3 EP0425088A3 (en) | 1992-06-17 |
EP0425088B1 true EP0425088B1 (en) | 1995-04-19 |
Family
ID=23685049
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP90310133A Expired - Lifetime EP0425088B1 (en) | 1989-10-23 | 1990-09-17 | Information storage in holograms |
Country Status (4)
Country | Link |
---|---|
US (1) | US5039182A (ja) |
EP (1) | EP0425088B1 (ja) |
JP (1) | JPH03146985A (ja) |
DE (1) | DE69018763D1 (ja) |
Families Citing this family (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5339305A (en) * | 1992-08-14 | 1994-08-16 | Northrop Grumman Corporation | Disk-based optical correlator and method |
US5963346A (en) * | 1997-12-12 | 1999-10-05 | Northrop Grumman Corporation | Scatter noise reduction in holographic storage systems by two-step write |
DE60227430D1 (de) * | 2001-04-04 | 2008-08-14 | Aprilis Inc | Speichersystem für Hybriddaten |
US7507504B2 (en) * | 2002-02-15 | 2009-03-24 | University Of Massachusetts | Optical storage system |
US7614203B2 (en) * | 2004-01-13 | 2009-11-10 | Safety Solutions, Inc. | User installable vacuum seal apparatus for storage bags |
DE102006005860A1 (de) | 2006-02-09 | 2007-08-30 | Bayer Innovation Gmbh | Verfahren und Vorrichtung zur Herstellung von Polarisationshologrammen |
US8284234B2 (en) | 2009-03-20 | 2012-10-09 | Absolute Imaging LLC | Endoscopic imaging using reflection holographic optical element for autostereoscopic 3-D viewing |
US10656596B2 (en) | 2014-10-09 | 2020-05-19 | EagleMae Ventures LLC | Video display and method providing vision correction for multiple viewers |
Family Cites Families (21)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US3544189A (en) * | 1968-06-12 | 1970-12-01 | Bell Telephone Labor Inc | Holography using a poled ferroelectric recording material |
US3627401A (en) * | 1969-02-24 | 1971-12-14 | Ibm | Binary-coded hologram recording system |
US3622220A (en) * | 1969-10-08 | 1971-11-23 | Bell Telephone Labor Inc | Holographic optical polarizers and beam splitters |
US3620589A (en) * | 1970-09-08 | 1971-11-16 | Bell Telephone Labor Inc | Interferometry of transparent objects |
JPS5121354B1 (ja) * | 1971-07-28 | 1976-07-01 | ||
JPS5123189B2 (ja) * | 1971-09-18 | 1976-07-15 | ||
US3698789A (en) * | 1971-10-20 | 1972-10-17 | Bendix Corp | Apparatus employing a grating to provide and move the source of a wave energy distribution |
BE790470A (fr) * | 1971-11-05 | 1973-04-24 | D Comp Gen | Procede et dispositif pour enregistrer des hologrammes superposes |
US3915549A (en) * | 1971-11-08 | 1975-10-28 | Rca Corp | Crystals for recording phase holograms |
US3825316A (en) * | 1972-04-24 | 1974-07-23 | Rca Corp | Apparatus for providing an optical system using adaptive holographic components |
US3891976A (en) * | 1974-01-14 | 1975-06-24 | Gte Laboratories Inc | Hologram memory with sequential data storage and beam angular relationship |
JPS544856B2 (ja) * | 1974-01-17 | 1979-03-10 | ||
FR2346810A1 (fr) * | 1976-03-30 | 1977-10-28 | Thomson Csf | Dispositif optique de stockage multiplie en volume |
FR2362466A1 (fr) * | 1976-08-19 | 1978-03-17 | Thomson Csf | Cellule d'enregistrement holographique, memoire et dispositif de calcul optique utilisant une telle cellule |
US4478481A (en) * | 1982-02-12 | 1984-10-23 | University Of Dayton | Production of diffraction limited holographic images |
US4720158A (en) * | 1983-12-07 | 1988-01-19 | Canon Kabushiki Kaisha | Method of and apparatus for making a hologram |
US4655542A (en) * | 1985-05-06 | 1987-04-07 | International Business Machines Corporation | Optical signal processing arrangements |
US4739496A (en) * | 1985-10-11 | 1988-04-19 | Hughes Aircraft Company | Associative holographic memory apparatus employing phase conjugate mirrors |
GB2203854B (en) * | 1987-04-21 | 1990-09-26 | Gen Electric Plc | Polarising optical device for forming a hologram. |
US4807970A (en) * | 1987-11-23 | 1989-02-28 | International Business Machines Corporation | Holograms in photorefractive materials |
US4830444A (en) * | 1987-12-31 | 1989-05-16 | American Telephone And Telegraph Company, At&T Bell Laboratories | Optical switch |
-
1989
- 1989-10-23 US US07/425,078 patent/US5039182A/en not_active Expired - Fee Related
-
1990
- 1990-08-28 JP JP2224565A patent/JPH03146985A/ja active Granted
- 1990-09-17 DE DE69018763T patent/DE69018763D1/de not_active Expired - Lifetime
- 1990-09-17 EP EP90310133A patent/EP0425088B1/en not_active Expired - Lifetime
Also Published As
Publication number | Publication date |
---|---|
EP0425088A3 (en) | 1992-06-17 |
EP0425088A2 (en) | 1991-05-02 |
JPH03146985A (ja) | 1991-06-21 |
US5039182A (en) | 1991-08-13 |
JPH0524518B2 (ja) | 1993-04-08 |
DE69018763D1 (de) | 1995-05-24 |
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